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Quark flavour observables in the Littlest Higgs model with T-parity after LHC Run 1

机译:LHC运行1之后在具有T奇偶校验的Littlest Higgs模型中可观察到夸克风味

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摘要

The Littlest Higgs model with T-parity (LHT) belongs to the simplest new physics scenarios with new sources of flavour and CP violation. The latter originate in the interactions of ordinary quarks and leptons with heavy mirror quarks and leptons that are mediated by new heavy gauge bosons. Also a heavy fermionic top partner is present in this model which communicates with the SM fermions by means of standard W± and Z0 gauge bosons. We present a new analysis of quark flavour observables in the LHT model in view of the oncoming flavour precision era. We use all available information on the CKM parameters, lattice QCD input and experimental data on quark flavour observables and corresponding theoretical calculations, taking into account new lower bounds on the symmetry breaking scale and the mirror quark masses from the LHC. We investigate by how much the branching ratios for a number of rare K and B decays are still allowed to depart from their SM values. This includes K+π+νν¯, KLπ0νν¯, KL → μ+μ-, B → Xsγ, Bs,d → μ+μ-, B → K(∗)+-, BK()νν¯, and ε/ε. Taking into account the constraints from ΔF = 2 processes, significant departures from the SM predictions for K+π+νν¯ and KLπ0νν¯ are possible, while the effects in B decays are much smaller. In particular, the LHT model favours ℬ(Bs → μ+μ-) ≥ ℬ(Bsμ+μ-)SM, which is not supported by the data, and the present anomalies in B → K(∗)+- decays cannot be explained in this model. With the recent lattice and large N input the imposition of the ε/ε constraint implies a significant suppression of the branching ratio for id="IEq17">KLπ0νν¯ with respect to its SM value while allowing only for small modifications of id="IEq18">K+π+νν¯. Finally, we investigate how the LHT physics could be distinguished from other models by means of indirect measurements and discuss the consequences for quark flavour observables of not finding any LHT state in the coming years.
机译:具有T奇偶校验(LHT)的Littlest Higgs模型属于最简单的新物理方案,具有新的味道和CP破坏源。后者起源于普通夸克和轻子与新的重玻色子介导的重镜夸克和轻子的相互作用。该模型中还存在一个重的费米离子顶级伴侣,该伴侣通过标准W ±和Z 0 玻色子与SM费米子通讯。鉴于即将到来的风味精度时代,我们对LHT模型中的夸克风味可观察物进行了新的分析。我们使用了有关CKM参数,晶格QCD输入和关于夸克风味可观察物的实验数据以及相应的理论计算的所有可用信息,同时考虑到LHC对称破损尺度和镜面夸克质量的新下限。我们研究了仍然允许多少罕见的K和B衰变的分支比偏离其SM值的程度。这包括 K + π + < / msup> ν ν ¯ K L π 0 ν < mrow> ν ¯ ,KL→μ + μ-,B→Xsγ,Bs,d→μ + μ - B →→ K (∗) + -,<数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML” id =“ M18”溢出=“滚动” > B K ∗ < / mo> ν <移动器accent =“ true”> ν ¯ 和< em>ε ' / ε。考虑到Δ F = 2过程的约束,与 K + < msup> π + ν <割> ν ¯ K < mi> L π 0 ν ν 是可能的,而 B 衰减中的影响要小得多。特别是LHT模型倾向于ℬ( B s μ + μ -)≥ℬ( B s μ + μ< / em> -)SM,该数据不受支持,并且 B K (∗)中存在当前异常 + -衰减在此模型中无法解释。对于最近的晶格和较大的 N 输入,ε ' / ε约束的施加意味着对 id =“ IEq17”> <数学xmlns:mml =“ http://www.w3.org/1998/Math/MathML”的分支比例“ id =” M34“ overflow =” scroll“> < msub> K L π 0 ν ν 的SM值,但仅允许 id =“ IEq18”> K + π + ν <移动器accent =“ true”> ν < / mrow> < / mrow> 。最后,我们研究了如何通过间接测量将LHT物理学与其他模型区分开来,并讨论了在未来几年未发现任何LHT状态对夸克风味可观察物的影响。

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